32493675d6
fixed bug in constitutive introduced in rev 2988 causing wrong names in *.outputConstitutive
2014-03-05 08:06:21 +00:00
a0d75ee05e
moved quaternion disorientation to lattice because it requires the knowledge of the lattice structure.
2014-02-28 13:28:27 +00:00
fe13bb16fe
added some consistency check and remove unnamed constants
2014-02-27 18:57:46 +00:00
69992638a8
added missing covera_ration in hex test. was not necessary before for constitutive_none, now it is
2014-02-17 09:45:54 +00:00
4efb1e5617
fixed bug: wrong initialization of lattice structure, had effect on j2 and phenopowerlaw
2014-02-14 18:05:59 +00:00
d45aea4467
moved reading in of lattice stru
2014-02-10 14:31:19 +00:00
9f3a17b1b6
fixed bug in hexagonal slip system definition
2014-01-15 12:08:46 +00:00
95d6430b09
improved on enums (introduced them for output in j2), fixed wrong recursion depth bug in IO, fixed a bug in reading in for none, j2, phenopowerlaw
2013-12-11 22:03:09 +00:00
7885ebaf8f
added 'reset' flag for recursive function IO_read, need to reset stack when stopping exectution (will be used by constitutive and homogenization)
2013-12-11 16:49:20 +00:00
0bc99a9622
change latticeName to latticeID
2013-11-27 16:20:27 +00:00
0a292d8d8b
fixed final bug in hex twintwin matrix
2013-10-15 22:02:39 +00:00
ed47d25adc
remove dotTemperature (returned always 0 anyway) to make it easier to replace it with a heating rate funtction
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remove potentially dangerous short circuiting in homogenization files
added doxygen comment for nonlocal (giving the functions a name)
fixed wrong definition of maxnchungs introcuded into dislotwin with last commit, causes trouble with hex
2013-10-09 06:12:16 +00:00
0a7052a7da
fixed two errors in hexagonal slipslip and twintwin interaction matrix
2013-10-08 13:52:19 +00:00
ce926aaf1f
Minor contribution :
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- add SVN keyword to the material.config file for cp-Ti
- add comments in lattice file
2013-09-19 09:17:09 +00:00
a8eb6a985e
- Addition of an example of a material.config file for hcp material (cp-Ti).
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- New Error Message #214 when elastic constants are not correctly defined.
- Error message when the c/a ratio for hcp is higher than 2 (no physical sense).
2013-09-17 12:20:50 +00:00
5f973a21c0
require all hardening coefficients/ non schmid coefficients to be specified in material.config, do not silently ignore any
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warning message now more meaningful (?) when using less than maximum number of slip families
2013-09-12 14:47:09 +00:00
39c05e0d9e
for bcc: exchanged 2nd and third hardening coefficient to be consistent with fcc; now 2nd is coplanar and 3rd is collinear; added newer reference concerning the bcc hardening coefficients
2013-08-14 11:47:03 +00:00
813ed130b0
nonSchmid behavior now ready to use for bcc with phenopowerlaw and nonlocal constitutive model.
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nonSchmid tensors according to Koester,Ma,Hartmaier,2012.
extended lattice_Sslip with non-Schmid tensors (the full non-symmetric tensors are required for the tangent and cannot be retrieved from the symmetrized Mandel notation)
2013-08-05 09:23:21 +00:00
3749cd5564
changed "math_AxisAngleToR" to "math_axisAngleToR" to be consistent with spelling in math.f90
2013-07-22 09:43:35 +00:00
8ccdfb27f3
reworked the hexagonal slip system order and adjusted interaction matrices to a logic that facilitates later system additions without altering existing structure.
2013-07-01 14:01:42 +00:00
4a291dc372
implementation of twin nucleation criteria according to Davids PhD thesis
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applies for fcc crystal structure only
2013-07-01 13:06:01 +00:00
81cdd2b1cc
added second type prismatic slip system for hexagonal lattices as 6th slip family.
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consequently, 4 new interaction types (21,22,23,24) available for slip/twin and twin/slip.
interaction of slip/slip got rearranged and now has 42 types...
list of former --> new:
6 7
7 8
8 9
9 10
10 11
11 13
12 14
13 15
14 16
15 18
16 19
17 20
18 22
19 23
20 25
21 28
22 29
23 30
24 31
25 33
26 34
27 35
28 37
29 38
30 40
2013-06-14 10:20:31 +00:00
85d4a37d95
moved public data res,size and homog from mesh to DAMASK_spectral_utilities (as grid and geomSize)
2013-05-08 15:52:29 +00:00
02f092492e
updated copyright header
2013-03-22 17:35:05 +00:00
3e2ecbe0a3
added time stamp to init of lattice
2013-03-07 22:45:00 +00:00
7e0ea5dd04
hickups in doxygen documentation fixed
2013-03-05 14:35:26 +00:00
62e55483f7
fixed bug in lattice: line continuation character was missing
2013-02-27 10:49:23 +00:00
bac186c5b7
removed 2003 standard initialization expression not supported by ifort so far
2013-02-27 07:35:53 +00:00
0be6706483
some more detailed doxygen comments
2013-02-26 19:01:31 +00:00
07ff1f7c93
reporting current time for most module inits
2013-02-25 16:34:59 +00:00
c1cf446774
parsing of material.config file now expects adequate number of (slip/twin) family entries according to given lattice type.
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used to read up to maxN, but that caused unnecessary IO_warnings...
2013-02-14 22:24:55 +00:00
e644c6dbc5
improved reading in of values, now only warnings in case of problematic entries in material.config
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divergence calculation sqrt scaling optionally introduced for basic scheme spectral solver
2013-02-08 15:55:53 +00:00
2b319f02e6
small corrections on changes related to non-schmid systems
2013-01-22 10:04:15 +00:00
60fec0e8ec
added code structure for non-schmid mechanics. work in progress…
2013-01-21 23:11:16 +00:00
fd94c786f0
moved stiffness tensor calculation to lattice
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introduced 'isotropic' and 'orthorhombic' lattice types to use corresponding symmetries in stiffness tensor. intended to be used with non-crystal plasticity models (j2, constitutive_none with isotropic, cubic or orthotropic elasticity).
2013-01-21 21:57:26 +00:00
1e32eb560e
corrected buggy calculation of Schmid matrix for twins introduced in rev1809.
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(stress acting on twin systems was overestimated by factor of sqrt(3) due to that!!)
additional polishing.
2012-11-23 17:02:50 +00:00
dc5cd8a4c4
A modified twin-twin interaction matrix for BCC is introduced.
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An introduction of a third parameter at the interactionTwinTwin in the material.config for BCC-dislotwin materials is essential.
2012-11-16 13:39:08 +00:00
c0a5a1dfd1
Formation of the Slip-Slip interaction matrix for BCC.
2012-11-14 17:35:33 +00:00
1896c07c70
corrected some bugs in the last commits
2012-11-14 14:33:41 +00:00
c8be3a03bd
The twin system <111>{112} for BCC is introduced.
2012-11-14 13:43:59 +00:00
6b010b4a46
Twin-slip interaction matrix for BCC is set to 0.
2012-11-14 11:53:22 +00:00
b0464ad176
A modified slip-twin interaction matrices for FCC and BCC are introduced.
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The shear twin value for BCC is corrected.
An introduction of a third parameter at the interactionSlipTwin in the material.config for dislotwin materials is essential.
2012-11-14 11:13:16 +00:00
fb2981b4c4
switched matrix indices in SlipSlip, SlipTwin, TwinSlip, and TwinTwin such that first index refers to first name and second to second...
2012-11-14 10:27:23 +00:00
79a5a30a90
removed now obsolete vectorproduct variables st, tt...
2012-10-18 07:25:49 +00:00
31f20e51da
just to be able to tell about the bug I found in the hex slip systems---which I actually forgot to mention during the last commit---I slipped in a syntax error that now is fixed, too...
2012-10-12 20:31:50 +00:00
82a13af474
tidied up the Schmid matrix calculations.
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added internal check against dilatation in Schmid matrices.
2012-10-12 17:59:50 +00:00
0bcb8f59db
added doxygen comments, some polishing, added "protected" statements where applicable
2012-10-02 12:53:25 +00:00
0434ef3daa
some comments to be seen in documentation
2012-08-15 13:38:38 +00:00
4d09ef0648
changed variable name "debug_what" to "debug_level"
2012-07-05 09:54:50 +00:00
dbdc7ddfa2
debug.config, debug.f90, DAMASK_abaqus_exp.f, DAMASK_abaqus_std.f: changed to new debug scheme (wasn't working)
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lattice.f90, FEsolving.f90: explicitly defined public functions and variables, all others are now private
numerics.f90: changed output format of real numbers, now instead of 0.1eX 1.0e(X-1) is printed to screen
Makefile: now using correct Optimization flags for OPTIMIZATION=AGGRESSIVE
DAMASK_spectral_AL.f90: improved, but still testing. Stress BCs now seem to be handled correctly
2012-03-20 18:01:31 +00:00
Martin Diehl